{"as_of":"2026-08-15T12:06:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:7974affd7f7309b91166119608345192a5b41cb7c3836af1c663968ed101010e","coverage":[{"denominator":59,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":59,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-14T05:26:30.717582Z","state":"measured"},{"denominator":61,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":61,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-15T06:32:42.880941+00:00","state":"measured"},{"denominator":2,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":2,"source":"paper_references, paper_reference_links","source_observed_at":"2026-05-11T01:31:07.210589Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"arxiv_reference","source_observed_at":"2026-05-11T01:45:51.362944Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"cited_work":{"arxiv_id":"1909.01370","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1909.01370","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","venue":null,"work_id":"30c0fa85-99f8-4d37-a6fa-8f997da7088a","year":2020},"citing_paper":{"arxiv_id":"2604.05044","last_updated":"2026-04-06T18:00:33Z","snapshot_observed_at":"2026-08-13T00:01:11.595051Z","submitted_at":"2026-04-06T18:00:33Z","title":"The chromomagnetic moment of a heavy quark with hyperasymptotic precision","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-05-10T19:19:14.408750Z"},"links":{"cited_paper":"/paper/1909.01370","citing_paper":"/paper/2604.05044"},"observation_digest":"sha256:673723762e886371892f1dd39a0ccde10ced0bfef5b554b964e82778134e3240","observation_id":"b419529f-9a30-48d5-adcb-704e8aad73e6","resolution":{"observed_at":"2026-05-10T23:10:50.584197Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"cited_work":{"arxiv_id":"1909.01370","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1909.01370","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","venue":null,"work_id":"30c0fa85-99f8-4d37-a6fa-8f997da7088a","year":2020},"citing_paper":{"arxiv_id":"2605.06996","last_updated":"2026-05-07T22:20:13Z","snapshot_observed_at":"2026-07-06T23:19:25.538514Z","submitted_at":"2026-05-07T22:20:13Z","title":"Renormalon-based resummation for B(D) Mesons","version":1},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-05-11T01:31:07.210589Z"},"links":{"cited_paper":"/paper/1909.01370","citing_paper":"/paper/2605.06996"},"observation_digest":"sha256:ba3aae328be556a3750f3a941704716ff26ed7371c725f8e4af22da16c4386a8","observation_id":"9db383b6-8649-4dbf-9763-f4a67efabb7e","resolution":{"observed_at":"2026-05-11T01:45:51.365173Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/1909.01370/citation-record","integrity":"/paper/1909.01370/integrity","json":"/paper/1909.01370/citation-record.json","paper":"/paper/1909.01370"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T05:26:31.776782Z","title":null,"venue":null,"work_id":"7b39ed71-2c6a-493c-a782-60593fa8cb89","year":2016},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.447721Z"},"links":{"citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:acf84a112de0384751f08037d8f7e4bb198195da11bfffc6feff27bda14d9289","observation_id":"000b8a0b-4af3-44b8-a3bd-a681303f2476","resolution":{"observed_at":"2026-08-14T05:26:31.781181Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T05:26:30.458437Z","title":null,"venue":null,"work_id":null,"year":1990},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.458437Z"},"links":{"citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:915d4598ef46f4e25e8b18b67cb8d3e392f827634bd76e8bb5d98c1d7e8cc17b","observation_id":"785c647a-372b-45bf-8f49-14859a51f060","resolution":{"observed_at":"2026-08-14T05:26:30.458437Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T05:26:31.790889Z","title":"6 for (b) mPV−mP−mΩm","venue":null,"work_id":"1503a702-7bc3-43cd-82d4-e780c58eabab","year":null},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.441479Z"},"links":{"citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:1cf1ab744eef1aff0d266c11550d3e9556dbdaa86eec611f7232c71e95746488","observation_id":"4aa22f5f-b807-414b-bfb7-46bfb37a9858","resolution":{"observed_at":"2026-08-14T05:26:31.796249Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1902.07736","last_updated":"2019-04-13T10:44:24Z","snapshot_observed_at":"2026-08-15T11:54:36.428575Z","submitted_at":"2019-02-20T19:14:46Z","title":"Superasymptotic and hyperasymptotic approximation to the operator product expansion","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1902.07736","snapshot_observed_at":"2026-08-14T05:26:30.453359Z","title":"Ayala, X","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.453359Z"},"links":{"cited_paper":"/paper/1902.07736","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:76f337ce2207ebaa8e2bee0a2c66a5ef5fcccce519c9970f33cb05a96a95f45e","observation_id":"0d85d124-9b85-4026-b526-4dd88f9da663","resolution":{"observed_at":"2026-08-14T05:26:30.453359Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T05:26:31.753986Z","title":null,"venue":null,"work_id":"a1487810-3f22-42ec-8098-cdb4eda47261","year":1999},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.462884Z"},"links":{"citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:872663196d80bcbcef11f5710607133ec31164e716d7f7799d31c9aaa0092c7e","observation_id":"2eff48fd-1f43-4581-bfb8-8b59c90c5db5","resolution":{"observed_at":"2026-08-14T05:26:31.758685Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1910.04090","last_updated":"2019-10-09T16:08:27Z","snapshot_observed_at":"2026-08-15T11:54:24.739653Z","submitted_at":"2019-10-09T16:08:27Z","title":"Hyperasymptotic approximation to the operator product expansion","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.04090","snapshot_observed_at":"2026-08-14T05:26:30.467239Z","title":"Ayala, X","venue":null,"work_id":null,"year":1910},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.467239Z"},"links":{"cited_paper":"/paper/1910.04090","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:33f6f088b7cbc88f93177fa323f255040e48711995e1ccba224f9be1510c90bf","observation_id":"e9fd6a4a-a9ec-4abf-949d-02573f49d903","resolution":{"observed_at":"2026-08-14T05:26:30.467239Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T05:26:31.739551Z","title":"Dingle, Asymptotic Expansions: Their Derivation and Interpretation (Academic Press, London, 1973)","venue":null,"work_id":"7582460a-ed05-4ea9-b46d-1b72fcb99af1","year":1973},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.472054Z"},"links":{"citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:1c3d60601604d6d363bb356a668a76e179b9409503430c819b04ab20a71fe998","observation_id":"7e2abd60-eccf-43da-8fad-57e3c6383b76","resolution":{"observed_at":"2026-08-14T05:26:31.744084Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T05:26:31.726375Z","title":"Tarrach, Nucl","venue":null,"work_id":"4d98efb3-50ca-4d1a-87e0-552181e32e29","year":1981},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.476626Z"},"links":{"citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:b8d518263bbb9f9c666ef964923e458d18a70e500a27704fff183121961463b9","observation_id":"f14dc46f-1a72-4b56-ae0f-a6c27f20fdae","resolution":{"observed_at":"2026-08-14T05:26:31.730596Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9907509","last_updated":"1999-07-27T10:01:32Z","snapshot_observed_at":"2026-08-11T05:05:19.165193Z","submitted_at":"1999-07-27T10:01:32Z","title":"Short Distance Mass of a Heavy Quark at Order \\alpha_s^3","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9907509","snapshot_observed_at":"2026-08-14T05:26:30.480710Z","title":null,"venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.480710Z"},"links":{"cited_paper":"/paper/hep-ph/9907509","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:1323fb7a6b33ed54466ceabcf09390ae77e886df78006ded3b6ebcf894468c80","observation_id":"f36afc73-ff63-4a7a-b5e2-c1f36878da7b","resolution":{"observed_at":"2026-08-14T05:26:30.480710Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9912391","last_updated":"2000-01-12T01:46:51Z","snapshot_observed_at":"2026-07-07T04:35:22.917311Z","submitted_at":"1999-12-17T03:35:46Z","title":"The three loop relation between the \\bar {MS} and the pole quark masses","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9912391","snapshot_observed_at":"2026-08-14T05:26:30.485438Z","title":"Melnikov and T","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.485438Z"},"links":{"cited_paper":"/paper/hep-ph/9912391","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:e8b83f179965afb32cc1ecfa47d64978e98b5a5b70ecc55d888bb88f8a451535","observation_id":"09fcfeaf-cd76-4d3a-aff3-28d3ac718cfe","resolution":{"observed_at":"2026-08-14T05:26:30.485438Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1502.01030","last_updated":"2015-04-30T13:24:45Z","snapshot_observed_at":"2026-08-14T23:01:30.276092Z","submitted_at":"2015-02-03T21:03:19Z","title":"Quark mass relations to four-loop order","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1502.01030","snapshot_observed_at":"2026-08-14T05:26:30.490253Z","title":"Marquard, A","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.490253Z"},"links":{"cited_paper":"/paper/1502.01030","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:a769dcab44c3af0794da4e19cf16f7b18c519ebf8a611dc6bd11a488d8152090","observation_id":"f7721212-9a4a-4453-ae4a-0e3f9abacd13","resolution":{"observed_at":"2026-08-14T05:26:30.490253Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9408380","last_updated":"1994-08-26T21:58:21Z","snapshot_observed_at":"2026-07-07T04:18:01.226236Z","submitted_at":"1994-08-26T21:58:21Z","title":"More on ambiguities in the pole mass","version":1},"cited_work":{"arxiv_id":"hep-ph/9408380","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9408380","snapshot_observed_at":"2026-08-14T05:26:31.606411Z","title":"More on ambiguities in the pole mass","venue":"hep-ph","work_id":"018270a6-10d2-41f2-8401-2e5b008619ab","year":1994},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.494563Z"},"links":{"cited_paper":"/paper/hep-ph/9408380","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:77cbe585c8b52ee8caa4c71c0bf34da19b11bca483284a9680c5e5c8af750677","observation_id":"e94c80fc-ee94-49e7-8f64-af7c90fe7bd6","resolution":{"observed_at":"2026-08-14T05:26:31.611299Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9807443","last_updated":"1999-01-01T13:40:48Z","snapshot_observed_at":"2026-08-10T06:38:05.295103Z","submitted_at":"1998-07-21T10:05:39Z","title":"Renormalons","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9807443","snapshot_observed_at":"2026-08-14T05:26:30.499367Z","title":"Beneke, Phys","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.499367Z"},"links":{"cited_paper":"/paper/hep-ph/9807443","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:539a96c8e8bff700be42d1fe0501b284f1425e9705ddcfa184640e55cb44b80d","observation_id":"53af134f-c8ed-427e-a16c-3f56fc36f426","resolution":{"observed_at":"2026-08-14T05:26:30.499367Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0105008","last_updated":"2001-06-28T15:26:01Z","snapshot_observed_at":"2026-07-07T03:52:16.194117Z","submitted_at":"2001-05-01T20:13:48Z","title":"Determination of the bottom quark mass from the $\\Upsilon(1S)$ system","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0105008","snapshot_observed_at":"2026-08-14T05:26:30.504451Z","title":"Pineda, JHEP 0106, 022 (2001) [hep-ph/0105008]","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.504451Z"},"links":{"cited_paper":"/paper/hep-ph/0105008","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:4a5c3d930cb3672a35f3c059c4a17acba1f7810bf67bc160d3159ee8770a9269","observation_id":"9ce2b097-bd35-431c-9506-23dd49c1b085","resolution":{"observed_at":"2026-08-14T05:26:30.504451Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1407.2128","last_updated":"2014-09-08T18:07:39Z","snapshot_observed_at":"2026-08-14T23:27:30.816155Z","submitted_at":"2014-07-08T15:12:09Z","title":"The bottom quark mass from the $\\Upsilon(1S)$ system at NNNLO","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1407.2128","snapshot_observed_at":"2026-08-14T05:26:30.509199Z","title":"Ayala, G","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.509199Z"},"links":{"cited_paper":"/paper/1407.2128","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:015cd2dad10a0e06ff22e5af4fc909df8104ff84449be846021e965b2ce3d79a","observation_id":"39f1cb92-5cac-43bf-af2f-c8fc85f173f3","resolution":{"observed_at":"2026-08-14T05:26:30.509199Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9205228","last_updated":"1992-05-21T18:16:09Z","snapshot_observed_at":"2026-08-10T07:31:32.340124Z","submitted_at":"1992-05-21T18:16:09Z","title":"Reparameterisation Invariance Constraints on Heavy Particle Effective Field Theories","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9205228","snapshot_observed_at":"2026-08-14T05:26:30.513799Z","title":null,"venue":null,"work_id":null,"year":1992},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.513799Z"},"links":{"cited_paper":"/paper/hep-ph/9205228","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:a43f692aacc2b41d8c795accba373154ea3fb8093c9a9e95bbce2dfb34211853","observation_id":"b39d0a5c-97d0-4183-a688-1ec6d20e1046","resolution":{"observed_at":"2026-08-14T05:26:30.513799Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9610471","last_updated":"1996-10-24T19:01:34Z","snapshot_observed_at":"2026-08-12T05:51:15.589361Z","submitted_at":"1996-10-24T19:01:34Z","title":"Exploring the Invisible Renormalon: Renormalization of the Heavy-Quark Kinetic Energy","version":1},"cited_work":{"arxiv_id":"hep-ph/9610471","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9610471","snapshot_observed_at":"2026-08-14T05:26:31.532982Z","title":"Exploring the Invisible Renormalon: Renormalization of the Heavy-Quark Kinetic Energy","venue":"hep-ph","work_id":"c05dbbd7-da08-4ea6-aa6a-e651de03fc8b","year":1996},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.518290Z"},"links":{"cited_paper":"/paper/hep-ph/9610471","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:70abfb75baa89712ed7961b46acac41157a997fc602922c2fbe1b18ae3e09613","observation_id":"848f7c55-1e0b-4f5e-8385-af6173ee3b5d","resolution":{"observed_at":"2026-08-14T05:26:31.537584Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0505034","last_updated":"2005-05-05T15:54:46Z","snapshot_observed_at":"2026-07-07T04:07:21.058548Z","submitted_at":"2005-05-05T15:54:46Z","title":"Static QCD Potential at r < 1/Lambda_QCD: Perturbative expansion and operator-product expansion","version":1},"cited_work":{"arxiv_id":"hep-ph/0505034","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0505034","snapshot_observed_at":"2026-08-14T05:26:31.513897Z","title":"Static QCD Potential at r < 1/Lambda_QCD: Perturbative expansion and operator-product expansion","venue":"hep-ph","work_id":"e395ac3c-5369-4f85-9db0-84c57402f4a6","year":2005},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.523183Z"},"links":{"cited_paper":"/paper/hep-ph/0505034","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:19c1e626bb939e18263b56cb5495f1e7cec21806c882ba29657e4703fa7fc33b","observation_id":"abbb5b3b-2c59-49fc-bdc9-7845833964a3","resolution":{"observed_at":"2026-08-14T05:26:31.518666Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0307070","last_updated":"2003-07-07T17:08:24Z","snapshot_observed_at":"2026-07-07T04:00:29.789829Z","submitted_at":"2003-07-04T17:21:20Z","title":"QCD perturbation theory at large orders with large renormalization scales in the large $\\beta_0$ limit","version":2},"cited_work":{"arxiv_id":"hep-ph/0307070","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0307070","snapshot_observed_at":"2026-08-14T05:26:31.494179Z","title":"QCD perturbation theory at large orders with large renormalization scales in the large $\\beta_0$ limit","venue":"hep-ph","work_id":"c075d307-464a-420e-965a-8608cd89b0f2","year":2003},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.527501Z"},"links":{"cited_paper":"/paper/hep-ph/0307070","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:4e6be393105858872673f76b16975600848e7c4222e38337998e226ebf06aafd","observation_id":"499fe763-81f8-4f9c-b2d0-e5f884af63f3","resolution":{"observed_at":"2026-08-14T05:26:31.499168Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9402364","last_updated":"1994-06-26T20:26:52Z","snapshot_observed_at":"2026-08-04T05:36:18.342230Z","submitted_at":"1994-03-01T01:56:11Z","title":"Heavy Quark Effective Theory beyond Perturbation Theory: Renormalons, the Pole Mass and the Residual Mass Term","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9402364","snapshot_observed_at":"2026-08-14T05:26:30.532637Z","title":"Beneke and V","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.532637Z"},"links":{"cited_paper":"/paper/hep-ph/9402364","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:e5dd6b3ac34d18634ae44f239962cd93b9ceb62a13cd0e8f4c7d6c52818d2b39","observation_id":"e13c3aca-540f-4955-9c5c-76f43a9c3261","resolution":{"observed_at":"2026-08-14T05:26:30.532637Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9502300","last_updated":"1995-02-14T16:08:12Z","snapshot_observed_at":"2026-08-10T11:48:46.857202Z","submitted_at":"1995-02-14T16:08:12Z","title":"Resummation of $(\\beta_0 \\alpha_s)^n$ Corrections in QCD: Techniques and Applications to the $\\tau$ Hadronic Width and the Heavy Quark Pole Mass","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9502300","snapshot_observed_at":"2026-08-14T05:26:30.537220Z","title":null,"venue":null,"work_id":null,"year":1995},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.537220Z"},"links":{"cited_paper":"/paper/hep-ph/9502300","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:a6a17e9a1d8b5e8c31091ecd64410fa6f3376912fd907e7721ab48a9936bff0d","observation_id":"e710161f-326f-4553-a7ad-8c414c766786","resolution":{"observed_at":"2026-08-14T05:26:30.537220Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9412265","last_updated":"1994-12-14T17:46:09Z","snapshot_observed_at":"2026-07-07T04:18:47.077477Z","submitted_at":"1994-12-09T10:23:47Z","title":"Scale Setting in QCD and the Momentum Flow in Feynman Diagrams","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9412265","snapshot_observed_at":"2026-08-14T05:26:30.542053Z","title":"Neubert, Phys","venue":null,"work_id":null,"year":1995},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.542053Z"},"links":{"cited_paper":"/paper/hep-ph/9412265","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:7c1c39dad5a8ac48a737d145bc05972ef268877916b2dc3b206b5f0b96d92049","observation_id":"78b1e4b5-e340-4679-927c-9709b7b75c25","resolution":{"observed_at":"2026-08-14T05:26:30.542053Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1111.3946","last_updated":"2012-05-25T18:27:16Z","snapshot_observed_at":"2026-08-15T04:28:43.018661Z","submitted_at":"2011-11-16T21:00:00Z","title":"Compelling evidence of renormalons in QCD from high order perturbative expansions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1111.3946","snapshot_observed_at":"2026-08-14T05:26:30.546230Z","title":"Bauer, G","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.546230Z"},"links":{"cited_paper":"/paper/1111.3946","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:5339dc6ee8d4c381439c87f1fb03f22d567a9c6b6181e88bcf0d5dee601803e0","observation_id":"95b25371-5b50-4399-963d-d5d2e05c8878","resolution":{"observed_at":"2026-08-14T05:26:30.546230Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1303.3279","last_updated":"2013-05-28T10:55:17Z","snapshot_observed_at":"2026-08-15T00:25:18.540834Z","submitted_at":"2013-03-13T20:10:49Z","title":"Perturbative expansion of the energy of static sources at large orders in four-dimensional SU(3) gauge theory","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1303.3279","snapshot_observed_at":"2026-08-14T05:26:30.551370Z","title":null,"venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.551370Z"},"links":{"cited_paper":"/paper/1303.3279","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:70c975f584607bfc6879c692a72b84ea81cca6556503fe1f3cb78f335d842e14","observation_id":"e5d56dc0-5a5a-4d51-be66-b4a19a67ceec","resolution":{"observed_at":"2026-08-14T05:26:30.551370Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1311.0114","last_updated":"2013-11-01T08:12:59Z","snapshot_observed_at":"2026-08-14T23:56:48.446787Z","submitted_at":"2013-11-01T08:12:59Z","title":"The static quark self-energy at O($\\alpha^{20}$) in perturbation theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1311.0114","snapshot_observed_at":"2026-08-14T05:26:30.555645Z","title":null,"venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.555645Z"},"links":{"cited_paper":"/paper/1311.0114","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:01b5e0b9eb6298f6bb7bc1e8a53416ec10d1c3d3b3fe046f4aab26aa146055e0","observation_id":"0b098f95-2a58-4d0a-bd93-5c37e4c503dc","resolution":{"observed_at":"2026-08-14T05:26:30.555645Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1904.02563","last_updated":"2019-06-27T08:43:22Z","snapshot_observed_at":"2026-08-14T16:51:43.622729Z","submitted_at":"2019-04-04T14:09:04Z","title":"UV contributions to energy of a static quark-antiquark pair in large $\\beta_0$ approximation","version":2},"cited_work":{"arxiv_id":"1904.02563","doi":null,"metadata_source":"pith","pith_arxiv_id":"1904.02563","snapshot_observed_at":"2026-08-14T05:26:31.393734Z","title":"UV contributions to energy of a static quark-antiquark pair in large $\\beta_0$ approximation","venue":"hep-ph","work_id":"73785d09-0648-42c1-989e-2efff799286b","year":2019},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.560749Z"},"links":{"cited_paper":"/paper/1904.02563","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:c3a4e30efe52d18054ae5636d21e58bebefc3eaeb864156a16aab805a2002ac3","observation_id":"cc33df6c-29e7-4320-828c-ceae236ef364","resolution":{"observed_at":"2026-08-14T05:26:31.398788Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T05:26:31.712621Z","title":"Hasenfratz and P","venue":null,"work_id":"6d7cfb88-b13b-4cb7-84a4-88a9421e9d07","year":1980},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.565883Z"},"links":{"citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:dd0fa9d8501cf25417f4cc2e91d9d25274d3a8526191fc57821bb188619901f6","observation_id":"6b8865de-e9ac-4040-85b3-1175a3eec0d3","resolution":{"observed_at":"2026-08-14T05:26:31.716934Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-lat/9405019","last_updated":"1994-05-24T12:42:36Z","snapshot_observed_at":"2026-07-07T03:44:32.747325Z","submitted_at":"1994-05-24T12:42:36Z","title":"Four Loop Result in $SU(3)$ Lattice Gauge Theory by a Stochastic Method: Lattice Correction to the Condensate","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-lat/9405019","snapshot_observed_at":"2026-08-14T05:26:30.570613Z","title":"Di Renzo, E","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.570613Z"},"links":{"cited_paper":"/paper/hep-lat/9405019","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:8702eb1b06d1bcb6e8cb9542fe526d1cface23ddbd9fbcc1be25be9469a35be7","observation_id":"91c25b59-440b-4089-ae0a-8606e1e353b2","resolution":{"observed_at":"2026-08-14T05:26:30.570613Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-lat/0410010","last_updated":"2004-12-23T15:25:50Z","snapshot_observed_at":"2026-07-07T03:42:34.907824Z","submitted_at":"2004-10-08T12:58:12Z","title":"Numerical Stochastic Perturbation Theory for full QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-lat/0410010","snapshot_observed_at":"2026-08-14T05:26:30.575088Z","title":"Di Renzo and L","venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.575088Z"},"links":{"cited_paper":"/paper/hep-lat/0410010","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:ff0926f268125ec7f061212bef6a04ed1f61ca461240f7cc9b5eb45eb6810cf0","observation_id":"932e47da-be11-4396-9fc3-1ba5226599d0","resolution":{"observed_at":"2026-08-14T05:26:30.575088Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-lat/0108008","last_updated":"2001-08-07T12:25:05Z","snapshot_observed_at":"2026-08-13T10:59:56.179852Z","submitted_at":"2001-08-07T12:25:05Z","title":"The Nf=0 heavy quark potential from short to intermediate distances","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-lat/0108008","snapshot_observed_at":"2026-08-14T05:26:30.579540Z","title":"Necco and R","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.579540Z"},"links":{"cited_paper":"/paper/hep-lat/0108008","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:04c6e576da6d47a40b111489ba69adc142e9d6d4583f5d32142528e930d68893","observation_id":"c76271f9-6522-424b-99b2-322553bec52d","resolution":{"observed_at":"2026-08-14T05:26:30.579540Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1403.6477","last_updated":"2014-08-15T12:20:14Z","snapshot_observed_at":"2026-08-14T23:39:58.922053Z","submitted_at":"2014-03-25T20:00:21Z","title":"Model-independent determination of the gluon condensate in four-dimensional SU(3) gauge theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1403.6477","snapshot_observed_at":"2026-08-14T05:26:30.583936Z","title":null,"venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.583936Z"},"links":{"cited_paper":"/paper/1403.6477","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:7aecf15b6e5ab8fd92eda2070848823365cbc4791ff725684c72d999a43ea2ff","observation_id":"4a1cdad5-6b18-4f45-b091-e01b611f153d","resolution":{"observed_at":"2026-08-14T05:26:30.583936Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-lat/9407025","last_updated":"1994-07-28T21:39:14Z","snapshot_observed_at":"2026-08-15T02:35:48.327319Z","submitted_at":"1994-07-28T21:39:14Z","title":"Properties of B-Mesons in Lattice QCD","version":1},"cited_work":{"arxiv_id":"hep-lat/9407025","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-lat/9407025","snapshot_observed_at":"2026-08-14T05:26:31.322442Z","title":"Properties of B-Mesons in Lattice QCD","venue":"hep-lat","work_id":"e2e2a167-37be-446f-9c46-f26107d07b23","year":1994},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.588473Z"},"links":{"cited_paper":"/paper/hep-lat/9407025","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:59296bd83424cda421ae46b1c3411f023c3c7778b91f828ddb8045bc24f99942","observation_id":"880ec07b-38ab-4229-8156-b648034c6eb6","resolution":{"observed_at":"2026-08-14T05:26:31.326798Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":"lat/9502013","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T05:26:31.300366Z","title":null,"venue":null,"work_id":"25ad4f5e-d998-4de7-904d-9e16d41273a2","year":1995},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.592682Z"},"links":{"citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:e59f3e3777b36ba2b6031533d0da62e93bed5a1d16707bfd1da511e3f400ff2e","observation_id":"48422aad-0597-4035-b3ab-3aca67c1c8e2","resolution":{"observed_at":"2026-08-14T05:26:31.307134Z","resolver_source":"raw_fallback","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-lat/9508030","last_updated":"1996-05-28T07:38:56Z","snapshot_observed_at":"2026-07-07T03:45:01.942164Z","submitted_at":"1995-08-29T17:40:26Z","title":"Heavy Quark Spectroscopy and Matrix Elements: A Lattice Study using the Static Approximation","version":2},"cited_work":{"arxiv_id":"hep-lat/9508030","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-lat/9508030","snapshot_observed_at":"2026-08-14T05:26:31.227546Z","title":"Heavy Quark Spectroscopy and Matrix Elements: A Lattice Study using the Static Approximation","venue":"hep-lat","work_id":"2d0a3625-fc24-492a-b6dc-b2d9c4790e75","year":1995},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.597969Z"},"links":{"cited_paper":"/paper/hep-lat/9508030","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:fb4d0a20cc98bf5c3ec597edc5379bd8353467d6562f65c3ec9ef2408cca0f44","observation_id":"2a3079a6-0b0e-499b-a65f-a6f285ec82fc","resolution":{"observed_at":"2026-08-14T05:26:31.232217Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0310130","last_updated":"2003-10-10T14:44:22Z","snapshot_observed_at":"2026-07-07T04:01:31.058013Z","submitted_at":"2003-10-10T14:44:22Z","title":"QCD phenomenology of static sources and gluonic excitations at short distances","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0310130","snapshot_observed_at":"2026-08-14T05:26:30.603064Z","title":null,"venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.603064Z"},"links":{"cited_paper":"/paper/hep-ph/0310130","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:54cf2384448c3cc23c0d95cb7bbd8d372fb44a382ccfb976e04263441d60a8b8","observation_id":"c36e5c7c-f18e-43d5-a203-4b1e9c58e359","resolution":{"observed_at":"2026-08-14T05:26:30.603064Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-lat/9208028","last_updated":"1992-08-27T11:04:40Z","snapshot_observed_at":"2026-08-15T01:14:50.459197Z","submitted_at":"1992-08-27T11:04:40Z","title":"Running Coupling and the Lambda-Parameter from SU(3) Lattice Simulations","version":1},"cited_work":{"arxiv_id":"hep-lat/9208028","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-lat/9208028","snapshot_observed_at":"2026-08-14T05:26:31.194586Z","title":"Running Coupling and the Lambda-Parameter from SU(3) Lattice Simulations","venue":"hep-lat","work_id":"ae2795d2-9248-4797-b3ff-a87b265e9d55","year":1992},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.607479Z"},"links":{"cited_paper":"/paper/hep-lat/9208028","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:16189182b7d3ce0bf07a6f61236d9b14bf4daacc48e6a30573be3a76311cbe26","observation_id":"4d82b208-30ec-4c41-98e8-8b177341ca25","resolution":{"observed_at":"2026-08-14T05:26:31.199376Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-lat/9703019","last_updated":"1997-03-27T13:51:45Z","snapshot_observed_at":"2026-07-07T03:45:45.698344Z","submitted_at":"1997-03-26T19:25:53Z","title":"Complete O(v^2) corrections to the static interquark potential from SU(3) gauge theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-lat/9703019","snapshot_observed_at":"2026-08-14T05:26:30.612004Z","title":null,"venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.612004Z"},"links":{"cited_paper":"/paper/hep-lat/9703019","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:d57fa0f9dd61668b0a7d062482e17f29d90798277558a1dd954666da5fd92495","observation_id":"2e5cd8ce-b4d1-4c3f-9833-7750b494449d","resolution":{"observed_at":"2026-08-14T05:26:30.612004Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1806.05197","last_updated":"2018-09-19T12:29:30Z","snapshot_observed_at":"2026-08-14T19:04:05.174909Z","submitted_at":"2018-06-13T18:00:29Z","title":"The charm/bottom quark mass from heavy quarkonium at N$^3$LO","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1806.05197","snapshot_observed_at":"2026-08-14T05:26:30.616405Z","title":"Peset, A","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.616405Z"},"links":{"cited_paper":"/paper/1806.05197","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:66d87c36d56c5e1abd86bcf7093a1d1adbff86e0f12e1838edb0965b55ba9d14","observation_id":"b9ae3464-7c06-4e41-a6a4-0091d20a8b46","resolution":{"observed_at":"2026-08-14T05:26:30.616405Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T05:26:30.620793Z","title":"Tanabashi et al","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.620793Z"},"links":{"citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:c6bb0b1fb7db42bec562b13d1c99f6216fd3a0b3ea4c5d69a6c83ebabb9a1f3b","observation_id":"2572ac93-167a-4e70-ab5b-dd392b37ca27","resolution":{"observed_at":"2026-08-14T05:26:30.620793Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1802.04248","last_updated":"2018-10-30T01:41:03Z","snapshot_observed_at":"2026-08-14T19:46:43.460397Z","submitted_at":"2018-02-12T18:57:23Z","title":"Up-, down-, strange-, charm-, and bottom-quark masses from four-flavor lattice QCD","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1802.04248","snapshot_observed_at":"2026-08-14T05:26:30.625010Z","title":"Bazavov et al","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.625010Z"},"links":{"cited_paper":"/paper/1802.04248","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:b1adfe07d8578808a2640771776a540f273dd886533bb36bcce3d3b56f1ed22f","observation_id":"03e6705d-44bf-475f-b6a8-71ad418073f7","resolution":{"observed_at":"2026-08-14T05:26:30.625010Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0304185","last_updated":"2003-11-05T06:15:56Z","snapshot_observed_at":"2026-08-13T15:47:01.944752Z","submitted_at":"2003-04-20T04:34:57Z","title":"Heavy quark mass determination from the quarkonium ground state energy: a pole mass approach","version":3},"cited_work":{"arxiv_id":"hep-ph/0304185","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0304185","snapshot_observed_at":"2026-08-14T05:26:31.134169Z","title":"Heavy quark mass determination from the quarkonium ground state energy: a pole mass approach","venue":"hep-ph","work_id":"7ceaf719-060c-45f5-8390-bcc3424f6ece","year":2003},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.629335Z"},"links":{"cited_paper":"/paper/hep-ph/0304185","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:c6f41f0a64214c6b66c536c059625bb2b27326c3c1fa868da2f204db2e490240","observation_id":"f9f83016-3534-4a5f-8ec7-63a94d065664","resolution":{"observed_at":"2026-08-14T05:26:31.139421Z","resolver_source":"local_arxiv","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0511238","last_updated":"2006-03-10T12:40:55Z","snapshot_observed_at":"2026-08-11T17:25:23.022859Z","submitted_at":"2005-11-20T03:12:14Z","title":"Constraining renormalon effects in lattice determination of heavy quark mass","version":3},"cited_work":{"arxiv_id":"hep-ph/0511238","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0511238","snapshot_observed_at":"2026-08-14T05:26:31.114107Z","title":"Constraining renormalon effects in lattice determination of heavy quark mass","venue":"hep-ph","work_id":"1b57bc25-0543-41d0-9452-ddc5ca12dbca","year":2005},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.633851Z"},"links":{"cited_paper":"/paper/hep-ph/0511238","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:9a5716a3a4d6a4fc855f6a0d2b85241b25a05fd9b64effa785eb4e16657df101","observation_id":"484f867a-1c96-4d48-a936-f5112ff06fb7","resolution":{"observed_at":"2026-08-14T05:26:31.119022Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1712.04983","last_updated":"2017-12-13T19:57:35Z","snapshot_observed_at":"2026-08-15T09:53:12.498373Z","submitted_at":"2017-12-13T19:57:35Z","title":"Relations between Heavy-light Meson and Quark Masses","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1712.04983","snapshot_observed_at":"2026-08-14T05:26:30.639173Z","title":"Brambilla et al","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.639173Z"},"links":{"cited_paper":"/paper/1712.04983","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:0530030b047b9dc7ad590aa89e70a0caf1c9fde2ff91d803cf9a3fe9c7aa2aed","observation_id":"b6a70afd-aa8e-42cd-930d-1788e933bcb3","resolution":{"observed_at":"2026-08-14T05:26:30.639173Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1701.00347","last_updated":"2017-09-30T21:16:47Z","snapshot_observed_at":"2026-08-14T21:22:54.032464Z","submitted_at":"2017-01-02T09:28:21Z","title":"A discussion on leading renormalon in the pole mass","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1701.00347","snapshot_observed_at":"2026-08-14T05:26:30.643938Z","title":"Komijani, JHEP 1708, 062 (2017) [arXiv:1701.00347 [hep-ph]]","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.643938Z"},"links":{"cited_paper":"/paper/1701.00347","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:a3183fdf0ce8a61ed5f7ba05f7fdd3fc9c13d095a858312f1b5cdad80ef720d6","observation_id":"a60a6767-423c-41e8-af29-f0d7e06d75b3","resolution":{"observed_at":"2026-08-14T05:26:30.643938Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9611010","last_updated":"1997-06-07T00:59:20Z","snapshot_observed_at":"2026-07-07T05:12:07.067291Z","submitted_at":"1996-11-03T15:59:20Z","title":"Renormalons Beyond One-Loop","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9611010","snapshot_observed_at":"2026-08-14T05:26:30.648260Z","title":"Lee, Phys","venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.648260Z"},"links":{"cited_paper":"/paper/hep-th/9611010","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:e03998e6ec3a2a074411b97fbab4cd554c419b46c213ff67eb6946b5959f2f4a","observation_id":"63a768aa-ef18-44bc-934c-4bb847d55ac6","resolution":{"observed_at":"2026-08-14T05:26:30.648260Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1704.01580","last_updated":"2018-04-05T13:41:54Z","snapshot_observed_at":"2026-08-15T04:53:59.555604Z","submitted_at":"2017-04-05T18:00:01Z","title":"The MSR Mass and the ${\\cal O}(\\Lambda_{\\rm QCD})$ Renormalon Sum Rule","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1704.01580","snapshot_observed_at":"2026-08-14T05:26:30.653495Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.653495Z"},"links":{"cited_paper":"/paper/1704.01580","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:fed7f7e7caa986a9b574e876b2454cdf3749f5a3ae9ce8ed6084be800316faa3","observation_id":"50730b3b-c159-45b5-843f-58598110bc64","resolution":{"observed_at":"2026-08-14T05:26:30.653495Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1605.03609","last_updated":"2017-06-09T15:55:52Z","snapshot_observed_at":"2026-08-14T21:57:46.213102Z","submitted_at":"2016-05-11T20:21:38Z","title":"On the ultimate uncertainty of the top quark pole mass","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1605.03609","snapshot_observed_at":"2026-08-14T05:26:30.657711Z","title":"Beneke, P","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.657711Z"},"links":{"cited_paper":"/paper/1605.03609","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:89c27c2986a563f13880e4fdd2a3a8d0d20b8ec99e5994897ebb16052c24f0f3","observation_id":"ee829bfa-4663-40ee-a3a7-30a44ba12a42","resolution":{"observed_at":"2026-08-14T05:26:30.657711Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1704.05095","last_updated":"2017-06-10T06:10:41Z","snapshot_observed_at":"2026-08-15T08:42:14.459606Z","submitted_at":"2017-04-17T18:59:25Z","title":"Comment on \"The MSR Mass and the ${\\cal O}(\\Lambda_{\\rm QCD})$ Renormalon Sum Rule\"","version":2},"cited_work":{"arxiv_id":"1704.05095","doi":null,"metadata_source":"pith","pith_arxiv_id":"1704.05095","snapshot_observed_at":"2026-08-14T05:26:31.026230Z","title":"Comment on \"The MSR Mass and the ${\\cal O}(\\Lambda_{\\rm QCD})$ Renormalon Sum Rule\"","venue":"hep-ph","work_id":"57775c8c-38c8-46a0-9dc9-f264a8b0bf56","year":2017},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.662021Z"},"links":{"cited_paper":"/paper/1704.05095","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:b1fb8b98fb4441f99fd0116628fee72c3057a6b15eeefeb1152984bf5be3e495","observation_id":"70c24f5c-ebfe-40df-b416-e1516a84fdfe","resolution":{"observed_at":"2026-08-14T05:26:31.031079Z","resolver_source":"local_arxiv","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1403.4427","last_updated":"2014-03-18T12:15:07Z","snapshot_observed_at":"2026-08-14T23:40:54.507704Z","submitted_at":"2014-03-18T12:15:07Z","title":"First combination of Tevatron and LHC measurements of the top-quark mass","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1403.4427","snapshot_observed_at":"2026-08-14T05:26:30.667384Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.667384Z"},"links":{"cited_paper":"/paper/1403.4427","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:25b594f9bab04d93074da9a8879d0bccaf417d3ce88e690025bf25ba2e6c5996","observation_id":"f4ee7435-e3d2-49ca-bcea-5cc2499dcdf9","resolution":{"observed_at":"2026-08-14T05:26:30.667384Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1509.04044","last_updated":"2016-04-14T14:38:30Z","snapshot_observed_at":"2026-08-14T22:32:32.901382Z","submitted_at":"2015-09-14T11:48:52Z","title":"Measurement of the top quark mass using proton-proton data at sqrt(s) = 7 and 8 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1509.04044","snapshot_observed_at":"2026-08-14T05:26:30.672975Z","title":"Khachatryan et al","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.672975Z"},"links":{"cited_paper":"/paper/1509.04044","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:6775bce5be34729e2fc6ace912710912eb745354c07f197d3db20f3a2ebe8948","observation_id":"fa413bd8-4c2a-46b9-b7cb-fe24bff77d7d","resolution":{"observed_at":"2026-08-14T05:26:30.672975Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1606.02179","last_updated":"2016-09-21T17:23:20Z","snapshot_observed_at":"2026-08-15T02:40:31.380894Z","submitted_at":"2016-06-07T15:22:36Z","title":"Measurement of the top quark mass in the $t\\bar{t}\\to$ dilepton channel from $\\sqrt{s}=8$ TeV ATLAS data","version":2},"cited_work":{"arxiv_id":"1606.02179","doi":null,"metadata_source":"pith","pith_arxiv_id":"1606.02179","snapshot_observed_at":"2026-08-14T05:26:30.977194Z","title":"Measurement of the top quark mass in the $t\\bar{t}\\to$ dilepton channel from $\\sqrt{s}=8$ TeV ATLAS data","venue":"hep-ex","work_id":"51ef9916-4ec3-4fde-9789-98007befacde","year":2016},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.677500Z"},"links":{"cited_paper":"/paper/1606.02179","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:9ccea2fc69c4fb6e0a133629dae61f33ddf1b33233db0ecc9155804d066db108","observation_id":"5cd311a9-e642-4e6e-a2f8-4e49a22e9b68","resolution":{"observed_at":"2026-08-14T05:26:30.982978Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1706.08526","last_updated":"2017-09-25T08:08:11Z","snapshot_observed_at":"2026-08-14T20:51:33.177817Z","submitted_at":"2017-06-26T18:00:01Z","title":"On the Light Massive Flavor Dependence of the Large Order Asymptotic Behavior and the Ambiguity of the Pole Mass","version":2},"cited_work":{"arxiv_id":"1706.08526","doi":null,"metadata_source":"pith","pith_arxiv_id":"1706.08526","snapshot_observed_at":"2026-08-14T05:26:30.957693Z","title":"On the Light Massive Flavor Dependence of the Large Order Asymptotic Behavior and the Ambiguity of the Pole Mass","venue":"hep-ph","work_id":"0ac45a04-fb20-4bfe-9350-4dc421818ac2","year":2017},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.682877Z"},"links":{"cited_paper":"/paper/1706.08526","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:77e7dda0e8b350b1e6ff6831030fba5ec4413c3a728c0e46a5304fa742760f35","observation_id":"ed8b822b-1661-4daf-a5f1-9b7e4525bc02","resolution":{"observed_at":"2026-08-14T05:26:30.962414Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1903.06574","last_updated":"2019-03-28T15:39:59Z","snapshot_observed_at":"2026-08-14T17:01:42.357737Z","submitted_at":"2019-03-15T14:35:07Z","title":"The top-quark mass: challenges in definition and determination","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1903.06574","snapshot_observed_at":"2026-08-14T05:26:30.687694Z","title":"Corcella, Front","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.687694Z"},"links":{"cited_paper":"/paper/1903.06574","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:17ea4d3fe74fc4fe32c603140d207e577e083349d8b671ba86e0fcafcaa56220","observation_id":"8a5d819a-6148-4bdc-a9d2-bed848f74b08","resolution":{"observed_at":"2026-08-14T05:26:30.687694Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9805215","last_updated":"1998-07-01T14:51:53Z","snapshot_observed_at":"2026-07-07T04:29:23.166685Z","submitted_at":"1998-05-04T22:15:03Z","title":"The Perturbative Pole Mass in QCD","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9805215","snapshot_observed_at":"2026-08-14T05:26:30.692922Z","title":null,"venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.692922Z"},"links":{"cited_paper":"/paper/hep-ph/9805215","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:824216a4c23ba5277d3189142c9ad6b17e0978452238ec2b543e9c31c9d7af04","observation_id":"e5e7b1c2-663f-475a-8dc0-6a9a262f382f","resolution":{"observed_at":"2026-08-14T05:26:30.692922Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T05:26:31.689425Z","title":null,"venue":null,"work_id":"dd43e48f-e36f-44b8-834f-6e9feefb2494","year":1990},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.698181Z"},"links":{"citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:aad8e904d6c6ece231a2ae959507a8b3ea59c3a709347b18db3b3f4169906d16","observation_id":"5b83bc65-7ade-481f-9a88-ce6c03c35c1d","resolution":{"observed_at":"2026-08-14T05:26:31.694968Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0708.1729","last_updated":"2007-08-13T16:07:00Z","snapshot_observed_at":"2026-08-15T10:34:19.537999Z","submitted_at":"2007-08-13T16:07:00Z","title":"Light quark mass effects in the on-shell renormalization constants","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0708.1729","snapshot_observed_at":"2026-08-14T05:26:30.703674Z","title":"Bekavac, A","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.703674Z"},"links":{"cited_paper":"/paper/0708.1729","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:db4bfdec8beaca063d8cfabb63cb9670cb2f4a7fdba1a5a6c509dbabad244401","observation_id":"df1125d9-f9fd-425d-b0d7-86ca498caf77","resolution":{"observed_at":"2026-08-14T05:26:30.703674Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1807.05406","last_updated":"2020-11-30T15:40:57Z","snapshot_observed_at":"2026-08-15T02:40:11.533697Z","submitted_at":"2018-07-14T15:05:34Z","title":"Multiloop contributions to the on-shell-$ \\overline{\\rm{MS}}$ heavy quark mass relation in QCD and the asymptotic structure of the corresponding series: the updated consideration","version":5},"cited_work":{"arxiv_id":"1807.05406","doi":null,"metadata_source":"pith","pith_arxiv_id":"1807.05406","snapshot_observed_at":"2026-08-14T05:26:30.897141Z","title":"Multiloop contributions to the on-shell-$ \\overline{\\rm{MS}}$ heavy quark mass relation in QCD and the asymptotic structure of the corresponding series: the updated consideration","venue":"hep-ph","work_id":"b737b81e-7ea6-4bf0-8167-99bb39fff4ae","year":2018},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.708154Z"},"links":{"cited_paper":"/paper/1807.05406","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:03cab8fca55b28e678ad4047d78a264e0fa57efb81b3d62ac5e98ce8cf894286","observation_id":"7d035f0e-328e-430e-a92e-b39c1a239b68","resolution":{"observed_at":"2026-08-14T05:26:30.903162Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1811.02867","last_updated":"2018-11-07T13:21:13Z","snapshot_observed_at":"2026-08-14T18:02:50.914047Z","submitted_at":"2018-11-07T13:21:13Z","title":"Dependence of five and six-loop estimated QCD corrections to the relation between pole and running masses of heavy quarks on the number of light flavours","version":1},"cited_work":{"arxiv_id":"1811.02867","doi":null,"metadata_source":"pith","pith_arxiv_id":"1811.02867","snapshot_observed_at":"2026-08-14T05:26:30.876076Z","title":"Dependence of five and six-loop estimated QCD corrections to the relation between pole and running masses of heavy quarks on the number of light flavours","venue":"hep-ph","work_id":"3801059b-5ecf-4978-b44c-bb355369f694","year":2018},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.712938Z"},"links":{"cited_paper":"/paper/1811.02867","citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:8f9438218ddb6ab2ff20d8af46565b0827eeaa466694df92a6b8a35137035eb7","observation_id":"d2f06269-58a4-45d8-9165-63d3598cb24d","resolution":{"observed_at":"2026-08-14T05:26:30.882477Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T05:26:30.717582Z","title":"Brambilla, A","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass","version":2},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-14T05:26:30.717582Z"},"links":{"citing_paper":"/paper/1909.01370"},"observation_digest":"sha256:c6f985b73c4f9235497314011a45138ced181500ca8f0b5d2514096026690ebd","observation_id":"53df4aae-5d2c-4887-8856-bb1b7f27a664","resolution":{"observed_at":"2026-08-14T05:26:30.717582Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"1909.01370","last_updated":"2020-02-10T19:04:29Z","latest_version":2,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-15T11:54:11.569196Z","submitted_at":"2019-09-03T18:00:12Z","title":"Hyperasymptotic approximation to the top, bottom and charm pole mass"},"reference_resolution":{"displayed":59,"state_counts":{"malformed_identifier":0,"metadata_mismatch":2,"parse_uncertain":0,"unresolved":39,"verified_exact":14,"verified_fuzzy":4},"total_outbound_references":59},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-15T06:32:42.880941+00:00","source":"crossref"},{"observed_at":"2026-08-15T06:32:39.529945+00:00","source":"retraction_watch"}],"thesis":"As of 15 August 2026, this Paper Citation Record lists 59 of 59 outbound references and 2 inbound Pith citation observations for arXiv:1909.01370."}